EXTRA CREDIT OPPORTUNITY: Due end of day, Thursday, Dec. 14

Size: px
Start display at page:

Download "EXTRA CREDIT OPPORTUNITY: Due end of day, Thursday, Dec. 14"

Transcription

1 EXRA CREDI OPPORUNIY: Due end of day, hursday, Dec. 4 his extra credit set of questions is an opportunity to improve your test scores (including an insurance policy for your final exam grade). here are 7 multiple choice questions in the following pages, each worth point. he points you receive for all questions answered correctly will be added to your total test score (including two midterms and the final). For example, if you received scores of 60 on midterm, 58 on midterm, and 70 on the final exam and answered all 7 extra credit questions correctly, your total point score for the exam component of the class would be: = 5, for a test average of 7.7 (this would be an improvement over your total test score without extra credit = 88, average = 6.7). he application of the extra credit will have a ceiling so that no one gets an average of over 00 for the three tests. Of course, if you are satisfied with your test scores you do not have to do any of these problems. Instructions: the questions are open book and notes, but they must be solved by you on your own. Show your work that justifies your answer. Questions involve some computation or explanation and you will not receive credit for an answer if you do not show your work or reasoning, i.e., there is no credit for guessing. If you have questions, see Prof. Hernandez or Silverstein. Please sign the honor code statement below before turning in the test, indicating that you have not received any unauthorized assistance. Do not worry if your answer is not exact. Select and circle the closest of the choices only one answer is correct for each question. Staple your worksheets to the exam, with the problems clearly numbered, when you turn it in. Name (print) I have read, understand, and agree to abide by the University of Colorado honor code in this test context: I have neither given nor received unauthorized assistance during this examination. Signed: Score: /7 points possible

2 . A vessel with a volume of m 3 contains liquid water and water vapor in equilibrium at 600 kpa. he liquid phase has a mass of kg. he mass of water vapor is: (a) 0.99 kg (b).6 kg (c).9 kg (d) 3. kg. he general equation for conservation of energy ( st Law) involves the following 5 terms: I. accumulation of energy in the control volume II. net energy transfer by work III. net energy transfer by heat IV. transfer of energy in by mass flow V. transfer of energy out by mass flow Using the standard sign conventions, which of the relations below is the correct arrangement of these terms that satisfies the st Law of hermodynamics? (a) I = II + III + IV V (b) I = II + III + IV + V (c) I = II + III + IV V (d) I = II III IV + V 3. In a reversible process, the state of a system changes from state to state as shown on the P- v diagram. What does the shaded area of the diagram represent? P v (a) free energy change (b) heat transfer (c) enthalpy change (d) boundary work

3 4. How much power is required to isothermally compress 3 m 3 /min of air from 0.5 kpa to 88.5 kpa? (a) 64 kw (b) 8 kw (c) 9 kw (d) 98 kw 5. Gas is in a closed piston-cylinder system. he gas is heated and expands from a volume of 0.04 m 3 to 0.0 m 3. he pressure varies such that the product P*v is constant, and the initial pressure is 00 kpa. What is the work done by the system? (a) 6.8 kj (b) 7.3 kj (c) 0 kj (d) kj 6. Steam flows into a turbine with the characteristics below at a rate of 0 kg/s and 0 kw of heat are lost from the turbine. Property inlet exit Pressure (MPa).0 0. emperature ( o C) Quality -- Neglecting potential and kinetic energy changes, what is the power output from the turbine? (a) 4,000 kw (b) 4,400 kw (c) 4,600 kw (d) 5,000 kw 7. How does an adiabatic process compare to an isentropic process? (a) adiabatic: heat transfer = 0; isentropic: heat transfer 0 (b) adiabatic: heat transfer 0; isentropic: heat transfer = 0 (c) adiabatic: reversible; isentropic: not reversible (d) both: heat transfer = 0; isentropic: reversible 8. An isobaric steam generating process starts with saturated liquid at 43 kpa ( s = 0 o C). he change in entropy during the steam generating process is EQUAL to the initial entropy (e.g., Δs = s ). Not all the liquid is vaporized. What is the change in enthalpy (Δh) during the process? (a) 300 kj (b) 46.3 kj/kg (c) 46.3 kj/kg (d) kj/kg 3

4 9. A piston-cylinder device contains saturated water vapor at 0 o C. he vapor is compressed in a reversible adiabatic process until the pressure is.6 MPa. What is the work done in the process? (a) 640 kj/kg (b) 50 kj/kg (c) 430 kj/kg (d) 330 kj/kg 0. For which type of process is the equation dq = ds valid? (a) irreversible (b) isothermal (c) reversible (d) isobaric. In the P-v diagram shown, heat addition to an ideal gas occurs in the process between states and. If c v for the gas is constant and = kj/kg-k. What is the entropy produced during this process. P : 3,78 kpa, 534K :,48 kpa, 600K (a) 0.4 kj/kg-k (b) 0.3 kj/kg-k (c) 0.3 kj/kg-k (d) 0.4 kj/kg-k v. An ideal reversible Carnot cycle is represented on the -S diagram below. he efficiency of the cycle is represented by which of the following ratios of areas? H L S 3 6 (a) (b) (c) (d)

5 3. In the Carnot cycle shown below, the net amount of heat put into the system is equal to the net amount of work done by the system. However, it cannot be stated that the heat put into the system between states and is equal to the work done between states and. What is the reason for this? 4 3 S (a) the process is adiabatic (b) the process is not adiabatic (c) the nd law states that the amount of energy put into the system is equal to the amount of energy taken out of the system (d) from the st law: dq = du + dw. It cannot be assumed that du = 0, so dq dw. 4. For a heat engine operating between two temperatures where ( > ), what is the maximum efficiency attainable? (a) (b) (c) (d) k 5. Steam expands from MPa and 00 o C to a mixture, x = 0.83 and 40 o C. What is the change in entropy of the steam? (a) 0.35 kj/kg-k (b) 0 kj/kg-k (c) 0.6 kj/kg-k (d) 0.73 kj/kg-k 6. Refrigerant (R-34a) is throttled in an adiabatic valve from h = 480 kj/kg and P = 0. MPa to a pressure of 0.06 MPa. What is the final enthalpy (h )? (a) 00 kj/kg (b) 300 kj/kg (c) 480 kj/kg (d) 560 kj/kg 5

6 7. he enthalpy of R-34a is reduced from 440 kj/kg to 300 kj/kg in a condenser maintained at 0.8 MPa (constant P). What is the final quality of the R-34a? (a) 3% (b) 37% (c) 63% (d) 7% 8. Steam enters an adiabatic steady-state nozzle at MPa, 50 o C, and 30 m/s. At one point in the nozzle the enthalpy has dropped to 40 kj/kg less than the inlet value. Determine the velocity of the steam at that point. (a) 3 m/s (b) 0 m/s (c) 50 m/s (d) 80 m/s 9. Air is compressed from 00 kpa and 40 o C to,500 kpa and 30 o C in a steady-flow process. During the compression process, each kilogram of air loses 90 kj as heat to the surroundings. Air is discharged at the rate of 0 m3/min. he required power input for the compressor is (a) 6 kw (b) 80 kw (c) 95 kw (d) 39 kw 0. Which of the following statements is the best interpretation of the st Law of hermodynamics for a closed system? (a) he mass within a closed control volume does not change (b) he net energy crossing the system boundary is the change in energy inside the system (c) he change in total energy of the system is equal to the rate of work performed (d) All real processes tend toward increased entropy in the universe -3. An ideal gas goes though a cycle consisting of three processes: A B: isothermal compression B C: isochoric cooling where C, P C =.4 bars and V C = 0.08 m 3 C A: isobaric expansion with net work = 0.5 kj. What is the volume at state A? (a) 0.07 m 3 (b) 0.0 m 3 (c) 0.9 m 3 (d) 0.4 m 3. What is the work in the process A B? (a) 9 kj (b) 3 kj (c) 0 kj (d) 5.3 kj 6

7 3. What is the net work of the cycle? (a) kj (b) 8.3 kj 6.5 kj (d) 4.8 kj 4. A steam pipe operating at steady-state receives 30 kg/min steam with an enthalpy of,900 kj/kg. If the enthalpy of the steam at the pipe exit equals,600 kj/kg, what is the rate of heat transfer from the pipe? (Neglect kinetic energy) (a) - 40 kj/min (b) kj/min (c) -,300 kj/min (d) - 39,000 kj/min 5. A flow of m 3 /min liquid oil is to be heated from 0 to 00 o C (stays as liquid) in a heat exchanger. he heating fluid is steam which enters the heat exchanger at 50 kpa and x = 0.9. he heat exchanger loses 5% of the heat transferred from the steam to the oil to the surroundings. he steam leaves the heat exchanger as saturated liquid. What is the mass flow rate of steam (kg/hr) required to heat the oil? (he density of the oil, ρ = 880 kg/m 3 and the specific heat =.00 kj/kg-k.) (a),00 kg/hr (b) 4,600 kg/hr (c) 8,600 kg/hr (d) 9,000 kg/hr 6. A refrigeration cycle has a coefficient of performance that is 80% of the Carnot refrigerator operating between temperature reservoirs at 33K and 68K. he rate of heat transfer from the low temperature reservoir is 3 kw. What is the required power input to the real refrigerator (not the Carnot refrigerator)? (a) 0.53 kw (b) 0.6 kw (c) 0.77 kw (d) 0.89 kw 7. An inventor claims that an engine produces 30 kw with a fuel consumption of 0 kg/hr. he energy content of the fuel transferred to the engine is 40,000 kj/kg when burned at 500 o C. Heat is rejected from the engine at 50 o C. Which laws of thermodynamics are violated by this claim? (a) First Law only (b) Second Law only (c) Both First and Second Laws (d) Neither First nor Second Laws 7

Chapters 5, 6, and 7. Use T 0 = 20 C and p 0 = 100 kpa and constant specific heats unless otherwise noted. Note also that 1 bar = 100 kpa.

Chapters 5, 6, and 7. Use T 0 = 20 C and p 0 = 100 kpa and constant specific heats unless otherwise noted. Note also that 1 bar = 100 kpa. Chapters 5, 6, and 7 Use T 0 = 20 C and p 0 = 100 kpa and constant specific heats unless otherwise noted. Note also that 1 bar = 100 kpa. 5-1. Steam enters a steady-flow device at 16 MPa and 560 C with

More information

ME ENGINEERING THERMODYNAMICS UNIT III QUESTION BANK SVCET

ME ENGINEERING THERMODYNAMICS UNIT III QUESTION BANK SVCET 1. A vessel of volume 0.04m 3 contains a mixture of saturated water and steam at a temperature of 250 0 C. The mass of the liquid present is 9 kg. Find the pressure, mass, specific volume, enthalpy, entropy

More information

a. The power required to drive the compressor; b. The inlet and output pipe cross-sectional area. [Ans: kw, m 2 ] [3.34, R. K.

a. The power required to drive the compressor; b. The inlet and output pipe cross-sectional area. [Ans: kw, m 2 ] [3.34, R. K. CHAPTER 2 - FIRST LAW OF THERMODYNAMICS 1. At the inlet to a certain nozzle the enthalpy of fluid passing is 2800 kj/kg, and the velocity is 50 m/s. At the discharge end the enthalpy is 2600 kj/kg. The

More information

Review Questions for the FE Examination

Review Questions for the FE Examination 110 THE FIRST LAW OF THERMODYNAMICS [CHAP. 4 4.1FE Review Questions for the FE Examination Select a correct statement of the first law if kinetic and potential energy changes are negligible. (A) Heat transfer

More information

LECTURE-15. Ideal Reverse Brayton Cycle. Figure (6) Schematic of a closed reverse Brayton cycle

LECTURE-15. Ideal Reverse Brayton Cycle. Figure (6) Schematic of a closed reverse Brayton cycle Lecturer: -Dr. Esam Mejbil Abid Subject: Air Conditioning and Refrigeration Year: Fourth B.Sc. Babylon University College of Engineering Department of Mechanical Engineering LECTURE-15 Ideal Reverse Brayton

More information

ESO 201A Thermodynamics

ESO 201A Thermodynamics ESO 201A Thermodynamics Instructor: Sameer Khandekar Tutorial 10 [8-23] A house that is losing heat at a rate of 50,000 kj/h when the outside temperature drops to 4 C is to be heated byelectric resistance

More information

Eng Thermodynamics I: Sample Final Exam Questions 1

Eng Thermodynamics I: Sample Final Exam Questions 1 Eng3901 - Thermodynamics I: Sample Final Exam Questions 1 The final exam in Eng3901 - Thermodynamics I consists of four questions: (1) 1st Law analysis of a steam power cycle, or a vapour compression refrigeration

More information

Second Law of Thermodynamics

Second Law of Thermodynamics Second Law of Thermodynamics Content Heat engine and its efficiency. Reversible and irreversible processes. The Carnot machine. Kelvin Planck Statement. Refrigerator and Coefficient of Performance. Statement

More information

CONTROL VOLUME ANALYSIS USING ENERGY. By Ertanto Vetra

CONTROL VOLUME ANALYSIS USING ENERGY. By Ertanto Vetra CONTROL VOLUME ANALYSIS USING ENERGY 1 By Ertanto Vetra Outlines Mass Balance Energy Balance Steady State and Transient Analysis Applications 2 Conservation of mass Conservation of mass is one of the most

More information

PAPER-I (Conventional)

PAPER-I (Conventional) 1. a. PAPER-I (Conventional) 10 kg of pure ice at 10 ºC is separated from 6 kg of pure water at +10 O C in an adiabatic chamber using a thin adiabatic membrane. Upon rupture of the membrane, ice and water

More information

B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering) B.Tech. (Aerospace Engineering) Term-End Examination

B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering) B.Tech. (Aerospace Engineering) Term-End Examination No. of Printed Pages : 5 ET-201(B) B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering) B.Tech. (Aerospace Engineering) Term-End Examination 007: 7 8 December, 2013 ET-201(B)

More information

OUTCOME 2 TUTORIAL 2 STEADY FLOW PLANT

OUTCOME 2 TUTORIAL 2 STEADY FLOW PLANT UNIT 47: Engineering Plant Technology Unit code: F/601/1433 QCF level: 5 Credit value: 15 OUTCOME 2 TUTORIAL 2 STEADY FLOW PLANT 2 Be able to apply the steady flow energy equation (SFEE) to plant and equipment

More information

flow work, p. 173 energy rate balance, p. 174 nozzle, p. 177 diffuser, p. 177 turbine, p. 180 compressor, p. 184 (4.4b) p. 166

flow work, p. 173 energy rate balance, p. 174 nozzle, p. 177 diffuser, p. 177 turbine, p. 180 compressor, p. 184 (4.4b) p. 166 0 Chapter 4 Control Volume Analysis Using Energy The use of mass and energy balances for control volumes at steady state is illustrated for nozzles and diffusers, turbines, compressors and pumps, heat

More information

In this lecture... Solve problems related to First law of thermodynamics for closed and open systems Heat engines Refrigerators and heat pumps

In this lecture... Solve problems related to First law of thermodynamics for closed and open systems Heat engines Refrigerators and heat pumps 13 1 In this lecture... Solve problems related to First law of thermodynamics for closed and open systems Heat engines Refrigerators and heat pumps 2 Problem 1 A 50 kg iron block at 80 C is dropped into

More information

Thermodynamics: Homework A Set 3 Jennifer West (2004)

Thermodynamics: Homework A Set 3 Jennifer West (2004) Thermodynamics: Homework A Set 3 Jennifer West (2004) Problem 1 In situations when only superheated steam is available a need for saturated steam arises. The required saturated steam can be obtained be

More information

MCG THERMODYNAMICS II. 22 April 2008 Page 1 of 7 Prof. W. Hallett

MCG THERMODYNAMICS II. 22 April 2008 Page 1 of 7 Prof. W. Hallett Faculté de génie Génie mécanique Faculty of Engineering Mechanical Engineering MCG2131 - THERMODYNAMICS II 22 April 2008 Page 1 of 7 Prof. W. Hallett Closed book. Non-programmable calculators only allowed.

More information

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT B.Tech. [SEM IV (ME-41, 42,43 & 44)] QUIZ TEST-1 (Session: )

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT B.Tech. [SEM IV (ME-41, 42,43 & 44)] QUIZ TEST-1 (Session: ) QUIZ TEST-1 Q.1. In a stage of an impulse turbine provided with a single row wheel, the mean diameter of the blade ring is 80cm and the speed of the rotation is 3000rpm. The steam issues from the nozzle

More information

Air Cycle Refrigeration Systems Nagendra M CBM Engineer, Hindusthan Zink.Ltd The specific objectives of the lesson This lesson discusses various gas cycle refrigeration systems based on air, namely: 1.

More information

MECHANICAL ENGINEERING THERMAL AND FLUID SYSTEMS STUDY PROBLEMS

MECHANICAL ENGINEERING THERMAL AND FLUID SYSTEMS STUDY PROBLEMS MECHANICAL ENGINEERING THERMAL AND FLUID SYSTEMS STUDY PROBLEMS PRINCIPLES: THERMODYNAMICS & ENERGY BALANCES 1 Copyright 2018. All rights reserved. How to use this book The exam specifications in effect

More information

Enhancement of CO2 Refrigeration Cycle Using an Ejector: 1D Analysis

Enhancement of CO2 Refrigeration Cycle Using an Ejector: 1D Analysis Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2006 Enhancement of CO2 Refrigeration Cycle Using an Ejector: 1D Analysis Elias

More information

Lecture No.3. The Ideal Reheat Rankine Cycle

Lecture No.3. The Ideal Reheat Rankine Cycle Lecture No.3 The Ideal Reheat Rankine Cycle 3.1 Introduction We noted in the last section that increasing the boiler pressure increases the thermal efficiency of the Rankine cycle, but it also increases

More information

UNIT NO-03 [8 hrs] Second Law Of Thermodynamics: Introduction (Law of degradation of energy), Thermal energy reservoirs, Kelvin-Plank & Clausius

UNIT NO-03 [8 hrs] Second Law Of Thermodynamics: Introduction (Law of degradation of energy), Thermal energy reservoirs, Kelvin-Plank & Clausius UNIT NO-03 [8 hrs] Second Law Of Thermodynamics: Introduction (Law of degradation of energy), Thermal energy reservoirs, Kelvin-Plank & Clausius statements, Heat engines, Refrigerator and Heat pump, Perpetual

More information

Exergy in Processes. Flows and Destruction of Exergy

Exergy in Processes. Flows and Destruction of Exergy Exergy in Processes Flows and Destruction of Exergy Exergy of Different Forms of Energy Chemical Energy Heat Energy Pressurised Gas Electricity Kinetic Energy Oxidation of Methane ΔH = -890.1 kj/mol ΔS

More information

Stationary Combustion Systems Chapter 6

Stationary Combustion Systems Chapter 6 Stationary Combustion Systems Chapter 6 Stationary combustion systems presently supply most of the earth s electricity. Conversion will take time, so study of these systems in order to improve them is

More information

Chapter 10 VAPOR AND COMBINED POWER CYCLES

Chapter 10 VAPOR AND COMBINED POWER CYCLES Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008 Chapter 10 VAPOR AND COMBINED POWER CYCLES Copyright The McGraw-Hill Companies, Inc. Permission

More information

Fluid Mechanics, Heat Transfer, Thermodynamics. Design Project. Production of Ammonia

Fluid Mechanics, Heat Transfer, Thermodynamics. Design Project. Production of Ammonia Fluid Mechanics, Heat Transfer, Thermodynamics Design Project Production of Ammonia Your assignment is to continue evaluating the details of a process to produce 50,000 tonne/y of ammonia from a syngas

More information

Consider a simple ideal Rankine cycle with fixed turbine inlet conditions. What is the effect of lowering the condenser pressure on

Consider a simple ideal Rankine cycle with fixed turbine inlet conditions. What is the effect of lowering the condenser pressure on Chapter 10, Problem 8C. Consider a simple ideal Rankine cycle with fixed turbine inlet conditions. What is the effect of lowering the condenser pressure on Pump work input: Turbine work output: Heat supplied:

More information

Fluid Mechanics, Heat Transfer, Fluid Mechanics Design Project. Production of Ethanol

Fluid Mechanics, Heat Transfer, Fluid Mechanics Design Project. Production of Ethanol Fluid Mechanics, Heat Transfer, Fluid Mechanics Design Project Production of Ethanol Your assignment is to continue evaluating the details of a process to produce 30,000 tonne/y of ethanol from ethylene.

More information

Engineering Thermodynamics

Engineering Thermodynamics Unit 61: Engineering Thermodynamics Unit code: D/601/1410 QCF level: 5 Credit value: 15 Aim This unit will extend learners knowledge of heat and work transfer. It will develop learners understanding of

More information

Performance Benefits for Organic Rankine Cycles with Flooded Expansion

Performance Benefits for Organic Rankine Cycles with Flooded Expansion Purdue University Purdue e-pubs Publications of the Ray W. Herrick Laboratories School of Mechanical Engineering 6-2-2010 Performance Benefits for Organic Rankine Cycles with Flooded Expansion Brandon

More information

Refrigeration Kylteknik

Refrigeration Kylteknik Värme- och strömningsteknik Thermal and flow engineering Refrigeration 424159.0 Kylteknik Ron Zevenhoven Exam 24-3-2017 4 questions, max. points = 4 + 6 + 10 + 10 = 30 All support material is allowed except

More information

Problems 2-9 are worth 2 points each. Circle T or F as appropriate for problems 6-9.

Problems 2-9 are worth 2 points each. Circle T or F as appropriate for problems 6-9. NAME KEY Allowed: Writing utensil, calculator and the provided formula sheet. Books, notes and collaboration (friends) are not allowed! Clearly indicate your answer and show your work. I do give partial

More information

Improvement of distillation column efficiency by integration with organic Rankine power generation cycle. Introduction

Improvement of distillation column efficiency by integration with organic Rankine power generation cycle. Introduction Improvement of distillation column efficiency by integration with organic Rankine power generation cycle Dmitriy A. Sladkovskiy, St.Petersburg State Institute of Technology (technical university), Saint-

More information

Combined Mass and Energy Transients

Combined Mass and Energy Transients Lecture T3 Combined Mass and Energy Transients We now consider processes in which the amounts of both mass and energy are changing in the system. In these cases, the material and energy balances are both

More information

Chapter 9: Applications of the Laws of Thermodynamics

Chapter 9: Applications of the Laws of Thermodynamics Chapter 9: Applications of the Laws of hermodynamics Goals of Period 9 Section 9.1: Section 9.2: Section 9.3: o review the first law of thermodynamics o discuss heat engines and their efficiency o discuss

More information

CHAPTER 2 POWER PLANT THERMODYNAMICS

CHAPTER 2 POWER PLANT THERMODYNAMICS CHAPTER 2 POWER PLANT THERMODYNAMICS 2.1. Thermodynamic Prciples... 2 2.2. Steady Flow Engeerg Devices and Processes... 4 2.3. Heat Enge and Cycles... 8 2.4. Carnot Cycle... 10 2.5. Ranke Cycle... 10 Chapter

More information

Fluid Mechanics, Heat Transfer, Thermodynamics Design Project. Production of Styrene

Fluid Mechanics, Heat Transfer, Thermodynamics Design Project. Production of Styrene Fluid Mechanics, Heat Transfer, Thermodynamics Design Project Production of Styrene The feasibility of constructing a new, grass-roots, 100,000 tonne/y, styrene plant is being investigated. As part of

More information

Michigan State University DEPARTMENT OF CHEMICAL ENGINEERING AND MATERIALS SCIENCE. ChE 321: Thermodynamics Spring 2017

Michigan State University DEPARTMENT OF CHEMICAL ENGINEERING AND MATERIALS SCIENCE. ChE 321: Thermodynamics Spring 2017 Michigan State University Name PID DEPARTMENT OF CHEMICAL ENGINEERING AND MATERIALS SCIENCE ChE 321: Thermodynamics Spring 2017 February 22, 2017, CLOSED NOTES Ver A. General Instructions Submit all problems

More information

A SUCCESSFUL INDUSTRY BASED AND ENERGY CONSERVATION RELATED SENIOR PROJECT. Frank Wicks Union College Schenectady, New York, 12308

A SUCCESSFUL INDUSTRY BASED AND ENERGY CONSERVATION RELATED SENIOR PROJECT. Frank Wicks Union College Schenectady, New York, 12308 A SUCCESSFUL INDUSTRY BASED AND ENERGY CONSERVATION RELATED SENIOR PROJECT Frank Wicks Union College Schenectady, New York, 12308 Session 2633 ABSTRACT The Mechanical Engineering program at Union College

More information

The Second Law of Thermodynamics

The Second Law of Thermodynamics The Second Law of Thermodynamics In this chapter we consider a more abstract approach to heat engine, refrigerator and heat pump cycles, in an attempt to determine if they are feasible, and to obtain the

More information

Principles of Engineering Thermodynamics. 8th Edition SI Version

Principles of Engineering Thermodynamics. 8th Edition SI Version Brochure More information from http://www.researchandmarkets.com/reports/3148694/ Principles of Engineering Thermodynamics. 8th Edition SI Version Description: Now in its Eighth Edition, Principles of

More information

Application of Exergy Analysis. Value and Limitations

Application of Exergy Analysis. Value and Limitations Application of Exergy Analysis Value and Limitations Power Plant Exergy Flows and Destruction Stack 2 Other Losses 1 Fuel 92 27 65 20 Steam 43 7 Shaft Power 32 Combustion Heat Transfer Turbine Steam 3

More information

Exergy Analysis of a Power Plant in Abu Dhabi (UAE)

Exergy Analysis of a Power Plant in Abu Dhabi (UAE) Exergy Analysis of a Power Plant in Abu Dhabi (UAE) Omar Mohamed Alhosani 1, Abdulla Ali Alhosani 2, Zin Eddine Dadach 3 1, 2, 3 Chemical Engineering Department, Abu Dhabi Men s College, Higher Colleges

More information

Applied Thermo Fluids-II: (Autumn 2017) Section-A: Thermal Power Plants

Applied Thermo Fluids-II: (Autumn 2017) Section-A: Thermal Power Plants Applied Thermo Fluids-II: (Autumn 2017) Section-A: Thermal Power Plants Module-1 (Introduction & Thermodynamics of thermal power plants) Dr. M. Ramgopal, Mechanical Engineering, IIT Kharagpur Reference:

More information

Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur (Refer Slide Time: 00:54) Lecture - 4 Second law of Thermodynamics

More information

OVERALL EFFICIENCY CONSIDERATION OF PNEUMATIC SYSTEMS INCLUDING COMPRESSOR, DRYER, PIPE AND ACTUATOR

OVERALL EFFICIENCY CONSIDERATION OF PNEUMATIC SYSTEMS INCLUDING COMPRESSOR, DRYER, PIPE AND ACTUATOR OVERALL EFFICIENCY CONSIDERATION OF PNEUMATIC SYSTEMS INCLUDING COMPRESSOR, DRYER, PIPE AND ACTUATOR Toshiharu KAGAWA*, Maolin CAI*, Hirotaka KAMEYA** *P recision and Intelligence Laboratory, Tokyo Institute

More information

Fluid Mechanics, Heat Transfer, Thermodynamics Design Project. Production of Ethylbenzene

Fluid Mechanics, Heat Transfer, Thermodynamics Design Project. Production of Ethylbenzene Fluid Mechanics, Heat Transfer, Thermodynamics Design Project Production of Ethylbenzene We continue to investigate the feasibility of constructing a new, grass-roots, 80,000 tonne/y, ethylbenzene facility.

More information

Thermodynamic Data. CO (g, 0 C, 1 atm) CO (g,100 C, 1 atm):

Thermodynamic Data. CO (g, 0 C, 1 atm) CO (g,100 C, 1 atm): Thermodynamic Data It is not possible to know the absolute value of Uˆ or Ĥ for a pure substance, but you can determine the change in U ˆ ( U ˆ ) or H ˆ ( Hˆ ) corresponding to a specified change of state

More information

Chapter 6 THE SECOND LAW OF THERMODYNAMICS

Chapter 6 THE SECOND LAW OF THERMODYNAMICS 6-1 Chapter 6 TE SECOND AW OF TERMODYNAMICS The Second aw of Thermodynamics and Thermal Energy Reservoirs 6-1C Water is not a fuel; thus the claim is false. 6-2C Transferring 5 kwh of heat to an electric

More information

[4163] T.E. (Mechanical) TURBO MACHINES (2008 Pattern) (Common to Mech. S/W) (Sem. - II)

[4163] T.E. (Mechanical) TURBO MACHINES (2008 Pattern) (Common to Mech. S/W) (Sem. - II) Total No. of Questions : 12] P1061 SEAT No. : [Total No. of Pages : 7 [4163] - 218 T.E. (Mechanical) TURBO MACHINES (2008 Pattern) (Common to Mech. S/W) (Sem. - II) Time : 3 Hours] [Max. Marks :100 Instructions

More information

Hydrogen oxygen steam generator integrating with renewable energy resource for electricity generation

Hydrogen oxygen steam generator integrating with renewable energy resource for electricity generation Available online at www.sciencedirect.com Energy Procedia 29 (2012 ) 12 20 World Hydrogen Energy Conference 2012 Hydrogen oxygen steam generator integrating with renewable energy resource for electricity

More information

St.MARTIN S ENGINEERING COLLEGE Dhulapally,Secunderabad,

St.MARTIN S ENGINEERING COLLEGE Dhulapally,Secunderabad, St.MARTIN S ENGINEERING COLLEGE Dhulapally,Secunderabad, 500014. MECHANICAL ENGINEERING TUTORIAL QUESTION BANK Course Name : THERMAL ENGINEERING II Course Code : A50326- Class : III B. Tech I Semester

More information

OPTIMIZATION OF PARAMETERS FOR HEAT RECOVERY STEAM GENERATOR (HRSG) IN COMBINED CYCLE PLANTS

OPTIMIZATION OF PARAMETERS FOR HEAT RECOVERY STEAM GENERATOR (HRSG) IN COMBINED CYCLE PLANTS OPTIMIZATION OF PARAMETERS FOR HEAT RECOVERY STEAM GENERATOR (HRSG) IN COMBINED CYCLE PLANTS Muammer Alus, Milan V. Petrovic University of Belgrade-Faculty of Mechanical Engineering, Laboratory of Thermal

More information

Thermodynamic analysis on post combustion CO 2 capture of natural gas fired power plant

Thermodynamic analysis on post combustion CO 2 capture of natural gas fired power plant Thermodynamic analysis on post combustion CO 2 capture of natural gas fired power plant Abstract Zeinab Amrollahi, 1 Ivar S. Ertesvåg, Olav Bolland Department of Energy and Process Engineering, Norwegian

More information

Refrigeration Cycle With Two-Phase Condensing Ejector

Refrigeration Cycle With Two-Phase Condensing Ejector Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2006 Refrigeration Cycle With Two-Phase Condensing Ejector Mark J. Bergander

More information

Feedwater Heaters (FWH)

Feedwater Heaters (FWH) Feedwater Heaters (FWH) A practical Regeneration process in steam power plants is accomplished by extracting or bleeding, steam from the turbine at various points. This steam, which could have produced

More information

2291-6A. Joint ICTP-IAEA Course on Science and Technology of Supercritical Water Cooled Reactors. 27 June - 1 July, 2011

2291-6A. Joint ICTP-IAEA Course on Science and Technology of Supercritical Water Cooled Reactors. 27 June - 1 July, 2011 2291-6A Joint ICTP-IAEA Course on Science and Technology of Supercritical Water Cooled Reactors 27 June - 1 July, 2011 INTRODUCTION TO THERMODYNAMICS Igor PIORO Faculty of Energy Systems and Nuclear Science

More information

K.S. Rawat 1, H. Khulve 2, A.K. Pratihar 3 1,3 Department of Mechanical Engineering, GBPUAT, Pantnagar , India

K.S. Rawat 1, H. Khulve 2, A.K. Pratihar 3 1,3 Department of Mechanical Engineering, GBPUAT, Pantnagar , India Thermodynamic Analysis of Combined ORC-VCR System Using Low Grade Thermal Energy K.S. Rawat 1, H. Khulve 2, A.K. Pratihar 3 1,3 Department of Mechanical Engineering, GBPUAT, Pantnagar-263145, India 2 Department

More information

CHAPTER 4 STEAM TURBINE and CYCLE HEAT BALANCE

CHAPTER 4 STEAM TURBINE and CYCLE HEAT BALANCE CHAPTER STEAM TURBINE and CYCLE HEAT BALANCE.1. Steam Turbine Principles... 2.2. Steam Turbine Analysis... 3.3. Arrangements of Steam Turbines..... Heat Balance... 6.. System Performance... 7 Chapter 1

More information

ENHANCEMENT OF COEFFICIENT OF PERFORMANCE IN VAPOUR COMPRESSION REFRIGERATION CYCLE

ENHANCEMENT OF COEFFICIENT OF PERFORMANCE IN VAPOUR COMPRESSION REFRIGERATION CYCLE ENHANCEMENT OF COEFFICIENT OF PERFORMANCE IN VAPOUR COMPRESSION REFRIGERATION CYCLE Dr Venkata Ramana Reddy Mula 1, H.V.Harish 2 1 Professor and Head, Department of Aeronautical Engineering NMIT BANGALORE

More information

Ejector Expansion Refrigeration Systems

Ejector Expansion Refrigeration Systems Research Inventy: International Journal Of Engineering And Science Vol.5, Issue 2 (February 2015), PP 25-29 Issn (e): 2278-4721, Issn (p):2319-6483, www.researchinventy.com Ejector Expansion Refrigeration

More information

SP1 Due by 4:30 pm EST on Friday 13 January 2017 to your division GradeScope site

SP1 Due by 4:30 pm EST on Friday 13 January 2017 to your division GradeScope site SP1 Due by 4:30 pm EST on Friday 13 January 2017 to your division GradeScope site The LED Helicopter is available online. It consists of a four-bladed pinwheel housing a battery and LED, along with a rubber

More information

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT B.Tech. [SEM IV (ME-41,42,43,44,45 & 46)] QUIZ TEST-2 (Session: 2012-13) APPLIED THERMODYNAMICS (EME-401) Q.1) In a gas turbine installation air is

More information

ES Fluid & Thermal Systems Page 1 of 6 STEAM TURBINE LABORATORY

ES Fluid & Thermal Systems Page 1 of 6 STEAM TURBINE LABORATORY ES 202 - Fluid & Thermal Systems Page 1 of 6 STEAM TURBINE LABORATORY Objective The objective of this laboratory experience is to demonstrate how mechanical power can be generated using a steam turbine

More information

STUDY OF CRYOGENIC CYCLES WITH ASPEN - HYSYS SIMULATIONS

STUDY OF CRYOGENIC CYCLES WITH ASPEN - HYSYS SIMULATIONS STUDY OF CRYOGENIC CYCLES WITH ASPEN - HYSYS SIMULATIONS A PROJECT REPORT SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF Bachelor of Technology in Mechanical Engineering By SUNIL

More information

Modeling and Investigation of Refrigeration System Performance with Two-Phase Fluid Injection in a Scroll Compressor

Modeling and Investigation of Refrigeration System Performance with Two-Phase Fluid Injection in a Scroll Compressor Marquette University e-publications@marquette Master's Theses (2009 -) Dissertations, Theses, and Professional Projects Modeling and Investigation of Refrigeration System Performance with Two-Phase Fluid

More information

ANALYSIS OF REFRIGERATION CYCLE PERFORMANCE WITH AN EJECTOR

ANALYSIS OF REFRIGERATION CYCLE PERFORMANCE WITH AN EJECTOR 000 (06) DOI:.5/ matecconf/067000 ICMER 05 ANALYSIS OF REFRIGERATION CYCLE PERFORMANCE WITH AN EJECTOR Wani J. R., Aklilu T. Baheta,a, Abraham D. Woldeyohannes, and Suhaimi Hassan Department of Mechanical

More information

Low-Grade Waste Heat Recovery for Power Production using an Absorption-Rankine Cycle

Low-Grade Waste Heat Recovery for Power Production using an Absorption-Rankine Cycle Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2010 Low-Grade Waste Heat Recovery for Power Production using an Absorption-Rankine

More information

Compact liquefied gas expander technological advances

Compact liquefied gas expander technological advances Compact liquefied gas expander technological advances Joel V. Madison President Ebara International Corporation SYNOPSIS LNG expanders are now an important part of every new LNG liquefaction plant. The

More information

Performance of a Gas Turbine Power Plant

Performance of a Gas Turbine Power Plant International Journal of Mechanical Engineering and Applications 2017; 5(1): 60-69 http://www.sciencepublishinggroup.com/j/ijmea doi: 10.11648/j.ijmea.20170501.18 ISSN: 2330-023X (Print); ISSN: 2330-0248

More information

Energy And Exergy Analysis Of Fully Condensing Steam Turbine At Various Steam Load Condition

Energy And Exergy Analysis Of Fully Condensing Steam Turbine At Various Steam Load Condition International Journal of ChemTech Research CODEN( USA): IJCRGG ISSN : 0974-4290 Vol.5, No.2, pp 957-963, April-June 2013 ICGSEE-2013[14 th 16 th March 2013] International Conference on Global Scenario

More information

Fluid Mechanics, Heat Transfer, Thermodynamics Design Project. Production of Formalin

Fluid Mechanics, Heat Transfer, Thermodynamics Design Project. Production of Formalin Fluid Mechanics, Heat Transfer, Thermodynamics Design Project Production of Formalin Your assignment is to continue evaluating the details of a process to produce 50,000 tonne/y of formalin. Formalin is

More information

Liquid-Flooded Ericsson Power Cycle

Liquid-Flooded Ericsson Power Cycle Purdue University Purdue e-pubs International Compressor Engineering Conference School of Mechanical Engineering 2014 Liquid-Flooded Ericsson Power Cycle Nelson A. James Purdue University, United States

More information

Chapter 6 THE SECOND LAW OF THERMODYNAMICS

Chapter 6 THE SECOND LAW OF THERMODYNAMICS Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008 Chapter 6 THE SECOND LAW OF THERMODYNAMICS Copyright The McGraw-Hill Companies, Inc. Permission

More information

ENGINEERING INFORMATION Hot water and steam service

ENGINEERING INFORMATION Hot water and steam service ENGINEERING INFORMTION Hot water and steam service What is steam? Like other substances, water can exist in the form of a solid, when we call it ice; as a liquid when we call it water or as a gas when

More information

Chapter 9. Two important areas of application for thermodynamics POWER AND REFRIGERATION CYCLES. Objectives

Chapter 9. Two important areas of application for thermodynamics POWER AND REFRIGERATION CYCLES. Objectives 99-R-online-chapter.qxd /9/07 : PM Page Chapter 9 POWER AD REFRIGERATIO CYCLES Two important areas of application for thermodynamics are power generation and refrigeration. Both power generation and refrigeration

More information

Cool Producing Systems Based on Burning and Gasification of Biomass

Cool Producing Systems Based on Burning and Gasification of Biomass Cool Producing Systems Based on Burning and Gasification of Biomass J. POSPISIL, J. FIEDLER, Z. SKALA Energy Institute Faculty of Mechanical Engineering Brno University of Technology Technicka 2, Brno

More information

Combined cycle with detailed calculation of Cp in the HRSG

Combined cycle with detailed calculation of Cp in the HRSG Combined cycle with detailed calculation of Cp in the HRSG A large, light-oil fired gas turbine with an electrical power output of 171 MW is integrated with a steam cycle, forming a combined cycle. Some

More information

Power cycles. Principles of combustion cycles and efficient concepts

Power cycles. Principles of combustion cycles and efficient concepts Power cycles Principles of combustion cycles and efficient concepts This contribution is based on the EC BREF- document Reference Document on Best Available Techniques for Large Combustion Plants July

More information

Investigation of Separator Parameters in Kalina Cycle Systems

Investigation of Separator Parameters in Kalina Cycle Systems Research Article International Journal of Current Engineering and Technology E-ISSN 2277 46, P-ISSN 2347-56 24 INPRESSCO, All Rights Reserved Available at http://inpressco.com/category/ijcet Investigation

More information

Basic Thermodynamics and System Analysis for Fuel Cells

Basic Thermodynamics and System Analysis for Fuel Cells 2 nd Joint European Summer School on Fuel Cell and Hydrogen Technology Crete, 17 th 28 th Sept. 2012 Basic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger-Wilckens Centre

More information

Energy Balances and Numerical Methods Design Project. Production of Methyl Tertiary-Butyl Ether

Energy Balances and Numerical Methods Design Project. Production of Methyl Tertiary-Butyl Ether Energy Balances and Numerical Methods Design Project Production of Methyl Tertiary-Butyl Ether Methyl Tertiary-Butyl Ether () is a gasoline additive used to increase octane number that is produced from

More information

Exergy Analysis of Vapor Compression Cycle

Exergy Analysis of Vapor Compression Cycle CHAPTER 4 Exergy Analysis of Vapor Compression Cycle 4.1 Introduction Refrigeration plays a very important role in industrial, domestic and commercial sectors for cooling, heating and food preserving applications.

More information

DEVELOPMENT OF TWIN PISTON EXPANDER WITH SOLENOID VALVE FOR ORGANIC RANKINE CYCLE

DEVELOPMENT OF TWIN PISTON EXPANDER WITH SOLENOID VALVE FOR ORGANIC RANKINE CYCLE 26-216 Asian Research Publishing Network (ARPN). All rights reserved. DEVELOPMENT OF TWIN PISTON EXPANDER WITH SOLENOID VALVE FOR ORGANIC RANKINE CYCLE Md. Nor Anuar Mohamad, Bukhari Manshoor, Mohd Faisal

More information

and Exergy Analysis of a Typical LiBr/H 2 O VAR

and Exergy Analysis of a Typical LiBr/H 2 O VAR CHAPTER - 3 Design and Evaluation of a 3 TR VAR System and Exergy Analysis of a Typical LiBr/H 2 O VAR System 3.1 Introduction The continuous increase in the cost and demand for energy has led to more

More information

Performance of a Combined Organic Rankine Cycle and Vapor Compression Cycle for Heat Activated Cooling

Performance of a Combined Organic Rankine Cycle and Vapor Compression Cycle for Heat Activated Cooling Performance of a Combined Organic Rankine Cycle and Vapor Compression Cycle for Heat Activated Cooling Hailei Wang*, Richard Peterson, Kevin Harada, Erik Miller, Robbie Ingram-Goble, Luke Fisher, James

More information

PERFORMANCE ANALYSIS OF ORGANIC RANKINE CYCLES USING DIFFERENT WORKING FLUIDS

PERFORMANCE ANALYSIS OF ORGANIC RANKINE CYCLES USING DIFFERENT WORKING FLUIDS THERMAL SCIENCE, Year 015, Vol. 19, No. 1, pp. 179-191 179 PERFORMANCE ANALYSIS OF ORGANIC RANKINE CYCLES USING DIFFERENT WORKING FLUIDS by Qidi ZHU, Zhiqiang SUN *, and Jiemin ZHOU School of Energy Science

More information

Chapter 8. Vapor Power Systems

Chapter 8. Vapor Power Systems Chapter 8 Vapor Power Systems Introducing Power Generation To meet our national power needs there are challenges related to Declining economically recoverable supplies of nonrenewable energy resources.

More information

Solutions to TUTORIAL-6 (10/03/2017) Thermodynamics for Aerospace Engineers (AS1300) Second Law of Thermodynamics

Solutions to TUTORIAL-6 (10/03/2017) Thermodynamics for Aerospace Engineers (AS1300) Second Law of Thermodynamics Solutions to TUTORIAL-6 (10/03/2017) Thermodynamics for Aerospace Engineers (AS1300) Second Law of Thermodynamics Q1. An inventor claims to have developed an engine that takes in 105 MJ at a temperature

More information

Revue des Energies Renouvelables Spécial ICT3-MENA Bou Ismail (2015) Numerical study of a single effect ejector-absorption cooling system

Revue des Energies Renouvelables Spécial ICT3-MENA Bou Ismail (2015) Numerical study of a single effect ejector-absorption cooling system Revue des Energies Renouvelables Spécial ICT3-MENA Bou Ismail (2015) 71-77 Numerical study of a single effect ejector-absorption cooling system D. Sioud 1*, M. Bourouis 2 et A. Bellagi 1 1 Unité de Recherche

More information

Investigation of New Low-GWP Refrigerants for Use in Two-Phase Evaporative Cooling of Electronics

Investigation of New Low-GWP Refrigerants for Use in Two-Phase Evaporative Cooling of Electronics Investigation of New Low-GWP Refrigerants for Use in Two-Phase Evaporative Cooling of Electronics Alexis Nicolette-Baker, Elizabeth Garr, Abhijit Sathe, and Steve O'Shaughnessey Precision Cooling Systems

More information

Efficiency improvement of steam power plants in Kuwait

Efficiency improvement of steam power plants in Kuwait Energy and Sustainability V 173 Efficiency improvement of steam power plants in Kuwait H. Hussain, M. Sebzali & B. Ameer Energy and Building Research Center, Kuwait Institute for Scientific Research, Kuwait

More information

The Effect of High Temperature Feedwater on the Performance of an Evaporative Cooler Installed in a Gas Turbine Combustion Air Inlet System

The Effect of High Temperature Feedwater on the Performance of an Evaporative Cooler Installed in a Gas Turbine Combustion Air Inlet System THE AMERICAN SOCIETY OF MECHANICAL ENGINEERS 345 E. 47th St, Now York. N.Y. 10017 96-GT-229 The Society shall not be responsible for statements or opinions advanced in papers or discussion at meetings

More information

The Reduced Pumping Power Requirements from Increasing the Injection Well Fluid Density

The Reduced Pumping Power Requirements from Increasing the Injection Well Fluid Density GRC Transactions, Vol. 37, 2013 The Reduced Pumping Power Requirements from Increasing the Injection Well Fluid Density Benjamin M. Adams 1, Thomas H. Kuehn 1, Jimmy B. Randolph 2, and Martin O. Saar 2

More information

Heat Transfer Theory. Jennie Borgström

Heat Transfer Theory. Jennie Borgström Heat Transfer Theory Jennie Borgström Modes of heat transfer Law of physics Heat = Energy If you take a hot spot and a cold spot the heat will always be transferred from the hot to the cold Three ways

More information

Development and Case Study of a Geothermal Power Generation System

Development and Case Study of a Geothermal Power Generation System Proceedings World Geothermal Congress 2015 Melbourne, Australia, 19-25 April 2015 Development and Case Study of a Geothermal Power Generation System Norihiro Fukuda 1, Katsuki Norito 1, Atsushi Fujii 1,

More information

Modeling of a Hot Gas Bypass Test Block for Centrifugal Compressors

Modeling of a Hot Gas Bypass Test Block for Centrifugal Compressors Purdue University Purdue e-pubs International Compressor Engineering Conference School of Mechanical Engineering 2014 Modeling of a Hot Gas Bypass Test Block for Centrifugal Compressors Paul D. Gessler

More information

COOLING TOWER DESIGN FOR CENTRAL GENERATORS OF CUET, BANGLADESH. Mohammad Sharif Khan, Golam Mainuddin, Abu Sadat Mohammad Sayem, Nadeem Nafis

COOLING TOWER DESIGN FOR CENTRAL GENERATORS OF CUET, BANGLADESH. Mohammad Sharif Khan, Golam Mainuddin, Abu Sadat Mohammad Sayem, Nadeem Nafis Proceedings of the 4 th BSME-ASME International Conference on Thermal Engineering 7-9 December, 008, Dhaka, Bangladesh COOLING TOWER DESIGN FOR CENTRAL GENERATORS OF CUET, BANGLADESH. Mohammad Sharif Khan,

More information

Qualitative Phase Behavior and Vapor Liquid Equilibrium Core

Qualitative Phase Behavior and Vapor Liquid Equilibrium Core 2/22/2017 Qualitative Phase Behavior and Qualitative Phase Behavior Introduction There are three different phases: solid, liquid, and gas (vapor) Energy must be added to melt a solid to form liquid If

More information

DSCC EFFECT OF MOISTURE ON THE EFFICIENCY AND POWER DENSITY OF A LIQUID PISTON AIR COMPRESSOR/EXPANDER

DSCC EFFECT OF MOISTURE ON THE EFFICIENCY AND POWER DENSITY OF A LIQUID PISTON AIR COMPRESSOR/EXPANDER Proceedings of the ASME 2016 Dynamic Systems and Control Conference DSCC2016 October 12-14, 2016, Minneapolis, Minnesota, USA DSCC2016-9884 EFFECT OF MOISTURE ON THE EFFICIENCY AND POWER DENSITY OF A LIQUID

More information